1. PHY 151: Lecture 4B 4.4 Particle in Uniform Circular Motion 4.5 Relative Velocity

2. PHY 151: Lecture 4B Motion in Two Dimensions 4.4 Particle in Uniform Circular Motion

3. Accelerated Motion No Acceleration  Object is at rest  Object is moving in a straight line with constant speed Acceleration  Object is moving in a straight line with changing speed  Object is moving in a curve with constant speed  Object is moving in a curve with changing speed

4. Uniform Circular Motion Uniform circular motion occurs when an object moves in a circular path with a constant speed The associated analysis model is a particle in uniform circular motion An acceleration exists since the direction of the motion is changing –This change in velocity is related to an acceleration The constant-magnitude velocity vector is always tangent to the path of the object

5. Changing Velocity in Uniform Circular Motion The change in the velocity vector is due to the change in direction The direction of the change in velocity is toward the center of the circle The vector diagram shows

6. Centripetal Acceleration - 1 The acceleration is always perpendicular to the path of the motion The acceleration always points toward the center of the circle of motion This acceleration is called the centripetal acceleration

7. Centripetal Acceleration - 2 The magnitude of the centripetal acceleration vector is given by The direction of the centripetal acceleration vector is always changing, to stay directed toward the center of the circle of motion

8. Period The period, T, is the time required for one complete revolution The speed of the particle would be the circumference of the circle of motion divided by the period Therefore, the period is defined as

9. Period - Example The tangential speed of a particle on a rotating wheel is 3.0 m/s Particle is 0.20 m from the axis of rotation How long will it take for the particle to go through one revolution?  d = vt  2  r = vT  T = 2  r/v = 2  (0.20)/3.0 = 0.42 s

10. Tangential Acceleration The magnitude of the velocity could also be changing In this case, there would be a tangential acceleration The motion would be under the influence of both tangential and centripetal accelerations –Note the changing acceleration vectors

11. Total Acceleration The tangential acceleration causes the change in the speed of the particle The radial acceleration comes from a change in the direction of the velocity vector

12. Total Acceleration, equations The tangential acceleration: The radial acceleration: The total acceleration: –Magnitude –Direction Same as velocity vector if v is increasing, opposite if v is decreasing

13. PHY 151: Lecture 4B Motion in Two Dimensions 4.5 Relative Velocity

14. Relative Velocity Two observers moving relative to each other generally do not agree on the outcome of an experiment However, the observations seen by each are related to one another A frame of reference can described by a Cartesian coordinate system for which an observer is at rest with respect to the origin

15. Different Measurements, example Observer A measures point P at +5 m from the origin Observer B measures point P at +10 m from the origin The difference is due to the different frames of reference being used.

16. Different Measurements, another example The man is walking on the moving beltway The woman on the beltway sees the man walking at his normal walking speed The stationary woman sees the man walking at a much higher speed. –The combination of the speed of the beltway and the walking The difference is due to the relative velocity of their frames of reference

17. Relative Velocity, generalized Reference frame SA is stationary Reference frame SB is moving to the right relative to SA at –This also means that SA moves at – relative to SB Define time t = 0 as that time when the origins coincide

18. Notation The first subscript represents what is being observed The second subscript represents who is doing the observing Example –The velocity of B (and attached to frame SB) as measured by observer A

19. Relative Velocity, equations The positions as seen from the two reference frames are related through the velocity – The derivative of the position equation will give the velocity equation – is the velocity of the particle P measured by observer A is the velocity of the particle P measured by observer B These are called the Galilean transformation equations

20. Acceleration in Different Frames of Reference The derivative of the velocity equation will give the acceleration equation The acceleration of the particle measured by an observer in one frame of reference is the same as that measured by any other observer moving at a constant velocity relative to the first frame

21. Acceleration, cont. Calculating the acceleration gives Since Therefore,